which we can identify as the entropy of \(\rho \)  relative to a uniform prior. Such alternatives are, however, ruled out in our scheme. This is not insignificant because the model of Bialynicki-Birula and Mycielski [1]} is still being used for the purposes of testing quantum theory (see e.g., [2]}), even despite its apparent conflict with relativity. Moreover, other choices available in the non-relativistic regime (see e.g., [3]}) also fail to be viable here. Thus the combination of ED and covariance is much more restrictive than many previous approaches to the issue of GQTs.
